Small separators, upper bounds for $l^\infty$-widths, and systolic geometry
Abstract: We investigate the dependence on the dimension in the inequalities that relate the Euclidean volume of a closed submanifold $Mn\subset \mathbb{R}N$ with its $l\infty$-width $W{l\infty}_{n-1}(Mn)$ defined as the infimum over all continuous maps $\phi:Mn\longrightarrow K{n-1}\subset\mathbb{R}N$ of $sup_{x\in Mn}\Vert \phi(x)-x\Vert_{l\infty}$. We prove that $W{l\infty}_{n-1}(Mn)\leq const\ \sqrt{n}\ vol(Mn){\frac{1}{n}}$, and if the codimension $N-n$ is equal to $1$, then $W{l\infty}_{n-1}(Mn)\leq \sqrt{3}\ vol(Mn){\frac{1}{n}}$. As a corollary, we prove that if $Mn\subset \mathbb{R}N$ is {\it essential}, then there exists a non-contractible closed curve on $Mn$ contained in a cube in $\mathbb{R}N$ with side length $const\ \sqrt{n}\ vol{\frac{1}{n}}(Mn)$ with sides parallel to the coordinate axes. If the codimension is $1$, then the side length of the cube is $4\ vol{\frac{1}{n}}(Mn)$. To prove these results we introduce a new approach to systolic geometry that can be described as a non-linear version of the classical Federer-Fleming argument, where we push out from a specially constructed non-linear $(N-n)$-dimensional complex in $\mathbb{R}N$ that does not intersect $Mn$. To construct these complexes we first prove a version of kinematic formula where one averages over isometries of $lN_\infty$ (Theorem 3.5), and introduce high-codimension analogs of optimal foams recently discovered in [KORW] and [AK].
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